Influence of Polymer Extensibility on the Temporal Stability Analysis of Planar Jet Flow in FENE-P Fluids

- 337743
Trabalho completo
Favoritar este trabalho
Como citar esse trabalho?
Resumo

This study extends the linear temporal stability analysis of incompressible, laminar, planar two-dimensional jet flows to viscoelastic fluids described by the FENE-P constitutive equation, extending beyond prior work restricted to the Oldroyd-B limit. The base flow is assumed steady and parallel, and the effects of the Reynolds number (Re), the Weissenberg number (Wi), the solvent viscosity ratio βn, and the maximum polymer extensibility L are assessed in terms of the growth rates of infinitesimal perturbations and the extent of unstable wavenumber regions, for both sinuous and varicose modes. Components of the conformation tensor A are obtained analytically for the Oldroyd-B limit and numerically for the full FENE-P model. Results show that inertia is destabilizing: increasing Re broadens the unstable region and raises peak temporal growth rates. Viscoelastic effects are generally stabilizing: higher Wi and larger L reduce both the unstable wavenumber range and maximum growth rates; however, this stabilizing influence of Wi is considerably weakened at low extensibility (L = 10), revealing a non-trivial interaction between polymer stretching and relaxation dynamics that is absent in the Oldroyd-B model.

Compartilhe suas ideias ou dúvidas com os autores!

Sabia que o maior estímulo no desenvolvimento científico e cultural é a curiosidade? Deixe seus questionamentos ou sugestões para o autor!

Faça login para interagir

Tem uma dúvida ou sugestão? Compartilhe seu feedback com os autores!

Instituições
  • 1 Universidade Estadual de Londrina
  • 2 Universidade Estadual Paulista (UNESP) - Presidente Prudente
  • 3 Instituto Nacional de Pesquisas Espaciais
  • 4 ICMC/USP, São Carlos, SP
Eixo Temático
  • ST05 - Física-Matemática, Mecânica dos Fluidos e Sistemas Dinâmicos
Palavras-chave
Jet Flow
Linear Stability Analysis
FENE-P model
Kelvin-Helmholtz instability